JPH0455251B2 - - Google Patents

Info

Publication number
JPH0455251B2
JPH0455251B2 JP12579185A JP12579185A JPH0455251B2 JP H0455251 B2 JPH0455251 B2 JP H0455251B2 JP 12579185 A JP12579185 A JP 12579185A JP 12579185 A JP12579185 A JP 12579185A JP H0455251 B2 JPH0455251 B2 JP H0455251B2
Authority
JP
Japan
Prior art keywords
conduit
axis
flow tube
inlet
outlet
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP12579185A
Other languages
Japanese (ja)
Other versions
JPS61283828A (en
Inventor
Akira Takada
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
OBARA KIKI KOGYO KK
Original Assignee
OBARA KIKI KOGYO KK
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by OBARA KIKI KOGYO KK filed Critical OBARA KIKI KOGYO KK
Priority to JP12579185A priority Critical patent/JPS61283828A/en
Publication of JPS61283828A publication Critical patent/JPS61283828A/en
Publication of JPH0455251B2 publication Critical patent/JPH0455251B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/76Devices for measuring mass flow of a fluid or a fluent solid material
    • G01F1/78Direct mass flowmeters
    • G01F1/80Direct mass flowmeters operating by measuring pressure, force, momentum, or frequency of a fluid flow to which a rotational movement has been imparted
    • G01F1/84Coriolis or gyroscopic mass flowmeters
    • G01F1/845Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits
    • G01F1/8468Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits vibrating measuring conduits
    • G01F1/8472Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits vibrating measuring conduits having curved measuring conduits, i.e. whereby the measuring conduits' curved center line lies within a plane
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/76Devices for measuring mass flow of a fluid or a fluent solid material
    • G01F1/78Direct mass flowmeters
    • G01F1/80Direct mass flowmeters operating by measuring pressure, force, momentum, or frequency of a fluid flow to which a rotational movement has been imparted
    • G01F1/84Coriolis or gyroscopic mass flowmeters
    • G01F1/845Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits
    • G01F1/8468Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits vibrating measuring conduits
    • G01F1/8472Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits vibrating measuring conduits having curved measuring conduits, i.e. whereby the measuring conduits' curved center line lies within a plane
    • G01F1/8477Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits vibrating measuring conduits having curved measuring conduits, i.e. whereby the measuring conduits' curved center line lies within a plane with multiple measuring conduits

Landscapes

  • Physics & Mathematics (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Volume Flow (AREA)

Description

【発明の詳細な説明】 1 産業上の利用分野 本願発明はコリオリの力を利用した質量流量計
に関する。
DETAILED DESCRIPTION OF THE INVENTION 1. Field of Industrial Application The present invention relates to a mass flowmeter that utilizes the Coriolis force.

2 従来技術 流管を流れる流体流に対して振動を与えると流
体流の流れの向きと、流管の振動軸とに対して直
角方向にコリオリの力が発生し、このコリオリの
力は振動周波数と流体の質量流量とに比例するこ
とが知られており、特開昭54−52570号公報にお
いてコリオリの力を利用した質量流量計が開示さ
れている。この従来例は支持部材に流入口及び流
出口部分をもつたU字形の導管を固着した本体形
状をもつており、流体は入口部よりU字形導管を
通つて流出する。U字形導管をU字形導管面(導
管のつくる面)に対して垂直の方向に支持部固着
線(流入口と流出口とが支持されている支持部を
結んだ線)を軸とした回転を与えると、U字形導
管を流れる流体にコリオリの力が作用し、固着線
に対して垂直なU字管軸に関してコリオリの力に
比例した捩じり振動が生ずる。このコリオリの力
を導管が基準面を通過する時間差から求めるよう
にしている。
2. Prior Art When vibration is applied to a fluid flow flowing through a flow tube, Coriolis force is generated in a direction perpendicular to the direction of the fluid flow and the vibration axis of the flow tube, and this Coriolis force is caused by vibration frequency. It is known that this is proportional to the mass flow rate of the fluid, and a mass flow meter using the Coriolis force is disclosed in Japanese Patent Application Laid-Open No. 54-52570. This conventional example has a body shape in which a U-shaped conduit having an inlet and an outlet portion is fixed to a support member, and fluid flows out from the inlet portion through the U-shaped conduit. Rotate the U-shaped conduit in a direction perpendicular to the U-shaped conduit surface (the surface on which the conduit is made) around the support fixing line (the line connecting the support where the inlet and outlet are supported). When applied, a Coriolis force acts on the fluid flowing through the U-shaped conduit, producing torsional vibrations proportional to the Coriolis force about the U-tube axis perpendicular to the anchor line. This Coriolis force is determined from the time difference when the conduit passes through the reference plane.

3 発明が解決しようとする問題点 上述の従来例はコリオリの力をU字形導管の捩
じり量として検出するものであるが該U字形導管
は導管面に垂直方向の振動が加えられる。しかし
取付上、導管面は水平か配管に平行して配設され
るので、前者においては床面の振動、後者におい
ては配管の横方向振動などの外乱に対して応動し
易く、更に、高感度に検出するための薄肉パイプ
を使用するので剛性が低く、これも外乱影響を受
け易くする原因となつており、S/N比の高い検
出を行うことが出来にくい面をもつている。
3 Problems to be Solved by the Invention In the conventional example described above, the Coriolis force is detected as the amount of twist of the U-shaped conduit, but the U-shaped conduit is subjected to vertical vibrations on the conduit surface. However, since the conduit surface is installed horizontally or parallel to the pipe, it is easy to react to disturbances such as floor vibration in the former case and lateral vibration of the pipe in the latter case, and also has high sensitivity. Since a thin-walled pipe is used for detection, its rigidity is low, which also makes it susceptible to external disturbances, making it difficult to perform detection with a high S/N ratio.

4 問題解決の手段 本願発明は上述の問題点を解決するためになさ
れたものである。即ち導管面を配管に直角方向に
することにより配管振動の影響を受け易い横方向
の導管剛性を高くするものである。
4. Means for solving the problem The present invention has been made in order to solve the above-mentioned problems. That is, by arranging the conduit surface perpendicular to the piping, the rigidity of the conduit in the lateral direction, which is susceptible to the effects of piping vibration, is increased.

5 実施例 第1図は本願発明の説明図であり、イは平面
図、ロは側面、ハは正面図で、1は流管であつて
該流管内は支切板6で流れを支切り、支切りの上
流と下流との間は導管2によつて連通してある。
導管2は、イ,ロ,ハの各図にしめすように、実
質上同一平面上で流管1を取囲むループ状になつ
ており、流入口21と流出口22とは各々流管壁
に開口し直径上のXX′でしめす第1軸に関し対称
位置にある。また流入口21、流出口22の近傍
の導管A,B部は第1軸とほぼ平行しており、導
管2が第1軸のまわりに流入口21および流出口
22を支点として回動可能となつている。また流
入口21および流出口22を結ぶ線YY′は第2軸
となり、該第2軸および第1軸に関し導管2は上
記A,B部を除き対称関係にある。支点7は必要
に応じて導管2を流管1に振動可能に軸支する。
5 Embodiments FIG. 1 is an explanatory diagram of the present invention, where A is a plan view, B is a side view, and C is a front view. , a conduit 2 communicates between the upstream and downstream sides of the split.
As shown in Figures A, B, and C, the conduit 2 has a loop shape that surrounds the flow tube 1 on substantially the same plane, and the inlet 21 and outlet 22 are formed on the flow tube wall. The opening is symmetrically located with respect to the first axis indicated by XX' on the diameter. In addition, the conduit A and B sections near the inlet 21 and the outlet 22 are approximately parallel to the first axis, and the conduit 2 can rotate around the first axis using the inlet 21 and the outlet 22 as fulcrums. It's summery. Further, the line YY' connecting the inlet 21 and the outlet 22 is a second axis, and the conduit 2 is symmetrical with respect to the second axis and the first axis, except for the above-mentioned portions A and B. The fulcrum 7 pivots the conduit 2 to the flow tube 1 in a oscillatory manner as required.

導管2を構成するループの第2軸上の位置に非
磁性体リング35を固着し、リング35に磁石3
が固着されている。該磁石3は、流管上に固着さ
れた支持台5に装着されたコイル4が導管の固有
振動数交流電源(図示省略)により励磁されるこ
とにより磁石3に対して吸引・反撥を繰返す。こ
の様子をロ図3−1,3−2の点線で示す。
A non-magnetic ring 35 is fixed to a position on the second axis of the loop constituting the conduit 2, and a magnet 3 is attached to the ring 35.
is fixed. The magnet 3 repeatedly attracts and repels the magnet 3 when a coil 4 attached to a support 5 fixed on the flow tube is excited by the natural frequency AC power source (not shown) of the conduit. This situation is shown by dotted lines in Figures 3-1 and 3-2.

流体は、流入口21より流入し、矢印のように
導管2をループにしたがつて流れ、流出口22か
ら支切板6の後流に流出する。導管2の振動がハ
図のX′方向に向く右ねじの方向の場合(即ちロ
図3−2の点線の場合)、導管m、M部はハ図に
おいて紙面に向かう変位が,n,N部において紙
面から手前側へコリオリの力が発生する。この力
の大きさは振動周波数が一定の場合、流体の質量
流量に比例する。また振動がX方向に向く右ねじ
の方向の場合(即ちロ図3−1の点線の場合)、
上述の反対の向きにコリオリの力を受ける。この
ことは、イ図2−1,2−2の点線のしめす交番
変位が生じることを意味し、これが駆動振動に加
算される形で、導管は第2軸のまわりに回転変位
する。この回転変位は図示しない検出器m,n,
又はM,Nに配設し、導管ループの静止面のよう
な基準面を通過する時間おくれとしてコリオリの
力である回転変位を計測して質量流量を求める。
また、流入口21、流出口22近傍のA,Bにお
いて、第2軸まわりの捩じり量を、該A,B部の
紙面表裏側でひずみゲージ等で検出することがで
きる。
The fluid flows in through the inlet 21, flows through the conduit 2 in a loop as shown by the arrow, and flows out through the outlet 22 downstream of the dividing plate 6. If the vibration of conduit 2 is in the direction of the right-hand screw facing in the Coriolis force is generated from the paper surface to the front side in the section. The magnitude of this force is proportional to the fluid mass flow rate for a constant vibration frequency. In addition, if the vibration is in the direction of the right-hand screw facing in the X direction (i.e., in the case of the dotted line in Figure 3-1),
Coriolis force is applied in the opposite direction to that described above. This means that an alternating displacement as shown by the dotted lines in FIGS. 2-1 and 2-2 occurs, and as this is added to the drive vibration, the conduit is rotationally displaced around the second axis. This rotational displacement is measured by detectors m, n, not shown,
Alternatively, the mass flow rate can be determined by disposing it at M and N and measuring the rotational displacement, which is the Coriolis force, at the time it takes to pass through a reference surface such as a stationary surface of the conduit loop.
Further, at A and B near the inlet 21 and the outlet 22, the amount of twist around the second axis can be detected using a strain gauge or the like on the front and back sides of the paper of A and B.

第2図は本願発明の他の実施例を示す。上記第
1図の実施例における導管2を第1導管とし、該
第1導管と同形等大の第2導管30を流管軸方向
に僅かに離間して配設し、第1導管2の第2軸上
の位置に非磁性リング35に固着された磁石3を
装着し、第2導管30の磁石3と対応する位置に
コイル4を装着し、該コイル4には導管の第1軸
まわりの固有振動数に実質的に等しい周波数の交
流電源(図示省略)により、磁石3に対して吸
引・反撥を繰返すことにより、各々第1、第2導
管は第1軸まわりに互いに反対位相で加振され
る。当然であるが、加振手段である磁石3とコイ
ル4との第1軸に関して対称点においては、加振
手段が吸引である場合には離間する。反対の場合
も成立する。加振手段側で反撥する場合について
のコリオリの力の発生をみると、導管2では第1
図ハと同様にM,m側で紙面に向かう方向、N,
n側では紙面から近づく方向となり、導管30で
は第1軸まわりの回転はXの向きとなり、上記導
管2の運動とは反対となる。即ちm側では近づ
き、n側では離間する方向の運動となり、次の半
周期では反対にm側が離間し、n側が近づく。こ
の場合も、コリオリの力は基準面を通過するm,
n点近傍に装着した図示しない「位置」又は「速
度検出」手段による信号から時間差として検出す
る。なお導管ループに正確な調和振動を与えるた
めXX′軸上の導管部を回転自在に支える支点7を
流管1に支持してもよい。
FIG. 2 shows another embodiment of the present invention. The conduit 2 in the embodiment shown in FIG. A magnet 3 fixed to a non-magnetic ring 35 is attached to a position on two axes, and a coil 4 is attached to a position corresponding to the magnet 3 of the second conduit 30. By repeatedly attracting and repelling the magnet 3 using an AC power source (not shown) with a frequency substantially equal to the natural frequency, each of the first and second conduits is excited around the first axis in opposite phases. be done. Naturally, at the point of symmetry between the magnet 3 and the coil 4, which are the excitation means, with respect to the first axis, they are separated when the excitation means is attraction. The opposite case also holds true. Looking at the generation of Coriolis force in the case of repulsion on the excitation means side, in conduit 2, the first
As in Figure C, M, direction toward the paper on the m side, N,
On the n side, the direction approaches from the plane of the paper, and in the conduit 30, the rotation around the first axis is in the X direction, which is opposite to the movement of the conduit 2. That is, the movement moves in the direction of approaching on the m side and moving away on the n side, and in the next half cycle, on the contrary, the m side moves away and the n side approaches. In this case as well, the Coriolis force passes through the reference plane m,
It is detected as a time difference from a signal by a "position" or "velocity detection" means (not shown) installed near point n. Note that in order to impart accurate harmonic vibration to the conduit loop, a fulcrum 7 that rotatably supports the conduit section on the XX' axis may be supported on the flow tube 1.

6 効果 以上説明した如く、本発明によれば、導管ルー
プの面は配管に対して直交する形となるので、配
管の剛性が弱いことにもとづいて生じる横方向の
振動に対して、導管のループの面が平行となり、
導管のループと直交する方向で検出するコリオリ
の力の信号方向に対して最も小さい振動影響のも
のが得られる。
6. Effects As explained above, according to the present invention, the surface of the conduit loop is perpendicular to the pipe, so that the conduit loop can withstand lateral vibrations that occur due to the low rigidity of the pipe. The planes of are parallel,
The least vibrational influence is obtained for the signal direction of the Coriolis force detected in the direction perpendicular to the conduit loop.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本願発明の一実施例を示し、イは平面
図、ロは側面図、ハは正面図を表す。第2図は他
の実施例である。 図中、1は流管、2,30は導管、3は磁石、
4はコイル、6は支切板を表す。
FIG. 1 shows an embodiment of the present invention, in which A is a plan view, B is a side view, and C is a front view. FIG. 2 shows another embodiment. In the figure, 1 is a flow tube, 2 and 30 are conduits, 3 is a magnet,
4 represents a coil, and 6 represents a dividing plate.

Claims (1)

【特許請求の範囲】 1 流管の流れを支切手段で支切つて得た上流側
から流入しかつ上記流管をループ状にとり囲み上
記支切手段の下流側に流出する導管をそなえ、該
導管を流管断面と実質上同一平面上におき、該導
管の流入口及び流出口の上記流管壁上の位置が流
管直径を軸としたとき第1軸に関し対称に近接し
て配置されると共に流入口、流出口近傍の導管を
所定区間ほぼ平行させ、上記導管を、第1軸に関
して対称でかつ流入口、流出口を結ぶ第2軸に関
して対称なループとなして流量計本体を構成し、
第1軸に関して調和運動をする加振手段を配設
し、第2軸まわりに発生するコリオリの力を検出
する検出手段をもうけ、該コリオリの力により質
量流量を計量することを特徴とする質量流量計。 2 上記におけるループ状導管は第1導管と、該
第1の導管に対して同形等大の第2導管とを流管
軸方向に僅かに離間して配設し、第1導管と第2
導管とを反対位相で加振する加振手段を配設した
ことを特徴とする第1項記載の質量流量計。
[Scope of Claims] 1. A conduit comprising a conduit that flows in from the upstream side obtained by dividing the flow of the flow tube with a dividing means, surrounds the flow tube in a loop shape, and flows out to the downstream side of the dividing means, and The conduit is placed substantially on the same plane as the flow tube cross section, and the positions of the inlet and outlet of the conduit on the flow tube wall are arranged symmetrically and close to each other with respect to a first axis when the flow tube diameter is the axis. At the same time, predetermined sections of the conduits near the inlet and outlet are made substantially parallel to each other, and the conduits are formed into a loop that is symmetrical with respect to a first axis and symmetrical with respect to a second axis that connects the inlet and outlet. death,
A mass characterized in that an excitation means that performs harmonic motion about a first axis is provided, a detection means is provided for detecting a Coriolis force generated around a second axis, and a mass flow rate is measured by the Coriolis force. Flowmeter. 2. The loop-shaped conduit described above has a first conduit and a second conduit of the same shape and size as the first conduit, which are arranged with a slight distance in the axial direction of the flow tube, and the first conduit and the second conduit are
2. The mass flowmeter according to claim 1, further comprising a vibrating means for vibrating the conduit in a phase opposite to that of the conduit.
JP12579185A 1985-06-10 1985-06-10 Mass flowmeter Granted JPS61283828A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12579185A JPS61283828A (en) 1985-06-10 1985-06-10 Mass flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12579185A JPS61283828A (en) 1985-06-10 1985-06-10 Mass flowmeter

Publications (2)

Publication Number Publication Date
JPS61283828A JPS61283828A (en) 1986-12-13
JPH0455251B2 true JPH0455251B2 (en) 1992-09-02

Family

ID=14918955

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12579185A Granted JPS61283828A (en) 1985-06-10 1985-06-10 Mass flowmeter

Country Status (1)

Country Link
JP (1) JPS61283828A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63231603A (en) * 1987-03-20 1988-09-27 Tokico Ltd flow control device

Also Published As

Publication number Publication date
JPS61283828A (en) 1986-12-13

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